Phase-noise reduction technique using frequency-to-current conversion with baseband integration
Abstract
A circuit for measurement of a phase noise of an oscillator may include the oscillator to generate a first signal having the same oscillation frequency as an instantaneous oscillation frequency of the oscillator. The circuit may include a first circuit that is configured to generate a second signal from the first signal. An instantaneous amplitude of the second signal may be related to the oscillation frequency of the first signal. A second circuit may be configured to integrate the second signal to generate a third signal. The third signal can be a measure of the phase noise of the oscillator. The third signal can be used to cancel some or all of the phase noise of the oscillator.
Claims
exact text as granted — not AI-modifiedWhat is claimed is:
1. A circuit for measurement of a phase noise of an oscillator, the circuit comprising:
a first circuit configured to generate a second signal from a first signal, wherein the first signal is generated by the oscillator at a frequency (ω c ) and includes a phase noise (φ n (t)) of the oscillator, and wherein an instantaneous amplitude of the second signal is proportional to a summation of the frequency (ω c ) of the first signal and a time derivative of the phase noise of the first signal (dφ n (t)/dt); and
a second circuit configured to integrate the second signal to generate a third signal, the third signal being a measure of the phase noise of the oscillator.
2. The circuit of claim 1 , wherein the first circuit is configured to utilize the first signal to generate at least one of a current signal or a voltage signal based on the oscillation frequency of the first signal.
3. The circuit of claim 1 , wherein the first circuit is a frequency-to-current converter circuit that is configured to utilize the first signal to generate a current signal based on the frequency of the first signal.
4. The circuit of claim 1 , wherein the first circuit is a frequency-to-voltage converter circuit that is configured to utilize the first signal to generate a voltage signal based on the frequency of the first signal.
5. The circuit of claim 1 , wherein the second circuit is configured to integrate the second signal and to eliminate an effect of the noiseless oscillation frequency on the third signal.
6. The circuit of claim 1 , wherein the second circuit comprises an integrator circuit configured to integrate the second signal and to substantially attenuate near-zero frequency signals.
7. The circuit of claim 1 , wherein the first circuit comprises a switched-capacitor circuit configured to utilize the first signal to generate at least one of a current signal or a voltage signal based on the oscillation frequency of the first signal.
8. The circuit of claim 7 , wherein the switches of the switched-capacitor circuit are controlled by the first signal and an inverted version of the first signal.
9. The circuit of claim 1 , wherein the first signal comprises a time varying voltage signal derived from an output signal of the oscillator.
10. A method for measurement of a phase noise of an oscillator, the method comprising:
deriving a first signal from the oscillator, wherein the first signal is generated by the oscillator at a frequency (ω c ) and includes a phase noise φ n (t)) of the oscillator; an instantaneous of the oscillator;
generating a second signal from the first signal, wherein an instantaneous amplitude of the second signal is proportional to a summation of the frequency (ω c ) of the first signal and a time derivative of the phase noise of the first signal (dφ n (t)/dt); and
integrating the second signal to generate a third signal, the third signal being a measure of the phase noise of the oscillator.
11. The method of claim 10 , wherein the generating of the second signal from the first signal comprises generating at least one of a current signal or a voltage signal based on the oscillation frequency of the first signal.
12. The method of claim 10 , wherein the generating of the second signal from the first signal comprises using a frequency-to-current converter circuit and utilizing the first signal to a generate a current signal based on the frequency of the first signal.
13. The method of claim 10 , wherein the generating of the second signal from the first signal comprises using a frequency-to-voltage converter circuit and utilizing the first signal to generate a voltage signal based on the frequency of the first signal.
14. The method of claim 10 , wherein the integrating of the second signal comprises eliminating an effect of the noiseless oscillation frequency on the third signal.
15. The method of claim 10 , wherein the integrating of the second signal comprises using an integrator that substantially attenuates near-zero frequency signals.
16. The method of claim 10 , wherein generating the second signal from the first signal comprises using a switched-capacitor circuit and utilizing the first signal to generate at least one of a current signal or a voltage signal based on the frequency of the first signal.
17. The method of claim 10 , wherein the deriving of the first signal from the oscillator comprises deriving a time varying voltage signal from an output signal of the oscillator.
18. The method of claim 10 , wherein generating the second signal comprises using a switched-capacitor circuit and configuring the switched-capacitor circuit to utilize the first signal to generate at least one of a current signal or a voltage signal or a current signal based on the oscillation frequency of the first signal.
19. A non-transitory machine-readable medium embodying instructions that, when executed by a machine, allow the machine to perform a method for measurement of a phase noise of an oscillator, the method comprising:
deriving a first signal from the oscillator, wherein the first signal is generated by the oscillator at a frequency ((ω c ) and includes a phase noise (φ n (t)) of the oscillator;
generating a second signal from the first signal, wherein an instantaneous amplitude of the second signal is proportional to a summation of the frequency (ω c ) of the first signal and a time derivative of the phase noise of the first signal (dφ n (t)/dt); and
integrating the second signal to generate a third signal, the third signal being a measure of the phase noise of the oscillator.
20. The non-transitory machine-readable medium of claim 19 , wherein:
a) the generating of the second signal from the first signal comprises generating at least one of a current signal or a voltage signal based on the frequency of the first signal, b) the generating of the second signal from the first signal comprises using a frequency-to-current converter circuit and utilizing the first signal to a generate a current signal based on the frequency of the first signal, and c) the integrating of the second signal comprises using an integrator that substantially attenuates near-zero frequency signals.Cited by (0)
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